1. Quasi-Elastic Scattering on MINERvA Kevin McFarland University of Rochester NuINT11, Dehradun 8 March 2011

2. To India via Indiana Thank you to the organizers for their efforts to allow me to attend my sister’s wedding (54 hours and 7500 miles ago) and still give this talk. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 2

3. Outline Goals and Strategies for Studies of (Quasi)- Elastic Scattering at MINERvA Scope of Our Initial Study Reconstruction and Data Selection Comparison with Simulations Outlook 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 3

4. Goals for (Quasi)-Elastic Scattering at MINERvA MINERvA was designed in large part to map out features of quasi- elastic cross-sections at moderate energies across a wide range of Q 2 –Broad range of energies, target nuclei 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 4 TargetLE ν μ Mass Scint. (CH)58.0K34.1K6.4t Helium2.6K1.3K0.25t Graphite (C)1.5K0.8K0.17t Water (H 2 O)3.2K2.2K0.4t Iron (Fe)9.5K4.3K0.97t Lead11.4K3.7K0.98t Fiducial CCQE Interactions/1.2E20 POT NuMI Beam MC, FLUKA

5. (Q)E Measurements Cross section for at low and moderate Q 2. –Also model-independent –Do we see similar enhancements at low energy seen by K2K, BooNEs? Agree with NOMAD at high energy? High Q 2 to extract axial form factors –Compare with vector form factors. Dipole? A-dependence of in nuclear targets for, particularly when NC elastic at moderate Q 2 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 5

6. MINERvA’s Prospects To illustrate our aspirations, here are our design- era simulation results for measurements with our full low energy data set. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 6 BooNEs NOMAD

7. MINERvA’s Prospects To illustrate our aspirations, here are our design- era simulation results for measurements with our full low energy data set. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 7 Statistical and resolution errors. No flux error. BooNEs NOMAD

8. Reconstruction Strategies One and Two- Track [SciBooNE, NOMAD] Work to lowest p p and widest θ p acceptance Worse in passive targets Lepton and Michel veto [“MiniBooNE” or Super-K] High energy will be challenging Only for scint. target One or Two Tracks plus no recoil (calorimetric) Today’s analysis from MINERvA Many possible approaches to QE reconstruction –Experiments choose approaches best suited to detector and beam energy. We hope to try all of these. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 8 Technique MINERvA- specific comments

9. MINERvA’s Challenges Dave Schmitz provided a detailed summary of MINERvA’s status –Increasing muon acceptance at low energy, will be critical for QEL Backgrounds –Each technique will have different non-elastic contributions –Higher energies are more challenging Flux uncertainties –See talk from Melissa Jerkins –We are pursuing techniques using neutrino interaction constraints and constraints independent of neutrinos 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 9 Z. Pavlovic, “A Measurement of Muon Neutrino Disappearance in the NuMI Beam,” PhD Thesis, UT Austin 2008

10. MINERvA’s First Quasi-Elastic Studies 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 10

11. Today’s Data Sample MINERvA’s run to date –Accumulated 0.8E20 with partial “frozen” detector in anti- neutrino mode –Accumulated 1.2E20 in neutrino and 1.3E20 in anti- neutrino beam with full detector This analysis is based on first half of partial detector anti-neutrinos in CH –About 10% of expected low energy anti-neutrinos 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 11 Full Detector “Frozen” Detector

12. Sample Events Muon is a long, penetrating track Neutron may or may not appear in the detector 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 12 Beam direction If elastic kinematics, E ν =2.8 GeV, Q 2 =0.1GeV 2 If elastic kinematics, E ν =2.5 GeV, Q 2 =0.3GeV 2 30 MeV deposited in single bar. Neutron interaction candidate. View of detector from above

13. Reconstruction and Data Selection 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 13

14. Muon Selection Analysis requires momentum analyzed muon in MINOS spectrometer Muon track must start in MINERvA detector Simulation everywhere is GENIE 2.6.2 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 14 Inclusive μ + originating in MINERvA, momentum analyzed in MINOS 3 ton fiducial mass

15. Recoil Selection Look at energy in the detector, outside of a region very close to the track (5cm) –Reduces contribution from δ-rays Form a calorimetric energy sum As expected, elastic events dominate at low recoil 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 15

16. Recoil vs Q 2 If the neutron interacts, may still see visible energy, particularly at high Q 2 (neutron energy) Our current selection varies with Q 2 Another option would be to require low recoil, eliminating signal with interacting neutrons 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 16

17. Backgrounds after Recoil 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 17 The current strategy is generous in keeping signal events, –at the price of leaving a significant background, particularly at high Q 2. This event illustrates two future background reduction techniques –Recoil energy near the track –Michel electron veto to remove π ±

18. Comparisons with Simulation 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 18

19. Technique for Comparison Uncertainties shown are from two sources –Data statistics and Simulation Statistics Simulation is approximately 2.5x the statistics of data –Flux uncertainties These uncertainties and the techniques for reducing them will be discussed in Melissa Jerkins’ talk Range from 7% at focusing peak to 16% at high energy –Other uncertainties (resolution, reconstruction efficiencies, material composition, etc.) not included Will show absolutely normalized comparisons –Except in plots to demonstrate agreement in “nuisance” variables, such as spatial distributions 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 19

20. selected Event location @ vertex 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 20 0.4E20 POT, partial detector

21. Muon location @ MINOS Good agreement in spatial distributions across detectors gives us confidence in our muon acceptance modeling 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 21 0.4E20 POT, partial detector

22. Muons in Selected Events Absolute normalization: protons + flux + cross-sections Recoil cut leaves Quasi-Elastic sample largely untouched, but reduces backgrounds significantly 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 22 Low Recoil 0.4E20 POT, partial detector Inclusive μ +

23. Efficiency of Reconstruction Reconstruction efficiency for true (generator) Quasi-Elastic –Biggest is loss of low energy muons –Slow fall of efficiency at high Q 2 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 23

24. Event Kinematics: Resolution 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 24 For true (generator) Quasi-Elastic events, look at resolution of event kinematics Derive neutrino energy and Q 2 from muon kinematics solely

25. Event Kinematics Reminder: absolute predictions from flux simulation, GENIE 2.6.2, MINERvA simulation Event deficit is flat in Q 2 and not flat in E ν 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 25 0.4E20 POT, partial detector

26. Outlook (Backdrop of beautiful vistas from much smaller hills) 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 26

27. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 27 Image © Barbie Marszalek 2009 The MINERvA detector is functioning well: reconstructed muons, calorimetric recoil Sufficient to take a first look at Quasi-Elastic Scattering

28. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 28 Image © Barbie Marszalek 2009 We have performed one (lonely) Quasi-Elastic analysis of many we plan for the future. Technique requires muon plus low recoil In the near future, will add proton reconstruction, lower energy muons, Michel veto. Cross-comparisons will help inform us about backgrounds

29. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 29 Image © Barbie Marszalek 2009 We’re looking forward to keeping this community involved in our long journey and welcome your comments and feedback.

30. Acknowledgments (from Monday’s MINERvA talk by Dave Schmitz) 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 30

31. 7 th International NuInt Workshop – March 7-11, 2011 – Dehradun, India Dave Schmitz, Fermilab 31 The MINER A Collaboration would like to sincerely thank many groups who have been critical to our progress so far: Fermilab Particle Physics Division for all their help installing the MINER A detector in the NuMI Near Detector Hall Fermilab Accelerator Division for their tireless efforts to keep the NuMI facility running and to provide intense beam since the detector was commissioned The ArgoNeuT Collaboration for paving the way for the use of cryogenic vessels in the underground area A very special thanks to the MINOS Collaboration for their willingness to share their data, so important to MINER A’s success, and for the significant effort required on the part of many collaborators to process, calibrate, and reconstruct the Near Detector samples which we use in our analysis Finally, we thank the Organizing Committee for NuInt 2011 for the opportunity to report on our progress and the status of our initial physics studies at this workshop! Thank You!

32. 7 th International NuInt Workshop – March 7-11, 2011 – Dehradun, India Dave Schmitz, Fermilab 32 The Collaboration is 100 members from 22 institutions in 7 countries HEP, Nuclear and Theory MINER A Collaboration

33. Backup Slides 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 33

34. 34 Generator Details GENIE 2.6.2 (tagged ~Jan 2011) Details of nucleon cross-section General equation is Llewellwyn-Smith with lepton mass terms The pseudo-scalar form factor is from PCAC. Electromagnetic form factors are BBBA2005 (hep-ex/0602017) Axial form factor has a dipole form, and M A =0.99 GeV/c 2. Nuclear effects (for carbon) The nuclear model is a Fermi gas, with a high momentum component (Bodek and Ritchie, Phys.Rev. D23 (1981) 1070). Pauli blocking is applied by requiring the outgoing nucleon has momentum above the Fermi momentum, 221 MeV/c for carbon. 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA

35. Event Kinematics 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 35, 0.4E20 POT, partial detector

36. Relatively Normalized Q 2 Distribution 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 36

37. Flux Uncertainty Detail 8 March 2011 K. McFarland, Quasi-Elastic @ MINERvA 37

38. 7 th International NuInt Workshop – March 7-11, 2011 – Dehradun, India Elevation View coming this Spring 5 m2 m LHe 0.25t 2.14 m 3.45 m Dave Schmitz, Fermilab 38 Full-Sized Detector Layout Detector comprised of 120 “modules” stacked along the beam direction Central region is finely segmented scintillator tracker ~32k readout channels total

39. 7 th International NuInt Workshop – March 7-11, 2011 – Dehradun, India Dave Schmitz, Fermilab 39 Full detector installation completed in March, 2010 NuMI beamline in low-energy configuration 1.2e20 P.O.T. in neutrino mode 1.2e20 P.O.T. in antineutrino mode Detector live-time > 98% Data Collected So Far